Statement

For ω∈K∞d\omega\in K_\infty^d, Tω([x])=[x+ω]T_\omega([x])=[x+\omega] on X=(K∞/OK)dX=(K_\infty/\mathcal O_K)^d with Haar probability is ergodic if and only if

Tr⁡∞(a⋅ω)∉Z(0≠a∈(OK∨)d).\operatorname{Tr}_\infty(a\cdot\omega)\notin\mathbb Z \qquad\bigl(0\ne a\in(\mathcal O_K^\vee)^d\bigr).
Fourier proof

Inverse pullback satisfies

αω(χa)=e−2πiTr⁡∞(a⋅ω)χa.\alpha_\omega(\chi_a)=e^{-2\pi i\operatorname{Tr}_\infty(a\cdot\omega)}\chi_a.

The is fixed exactly when its trace pairing is integral. Character completeness gives the fixed-function criterion.

Equivalent integral-coefficient test

The same ergodicity test can quantify over 0≠k∈OKd0\ne k\in\mathcal O_K^d. Indeed, OK⊆OK∨\mathcal O_K\subseteq\mathcal O_K^\vee, and multiplying a violating codifferent frequency by an integer NN with NOK∨⊆OKN\mathcal O_K^\vee\subseteq\mathcal O_K produces a violating integral frequency. This does not change which lattice indexes all Fourier characters.

Distinction from a ring action

The condition k⋅ω∉OKk\cdot\omega\notin\mathcal O_K for nonzero integral kk is instead the criterion for the . It is insufficient for one translation in higher-degree fields.